CN111367064B - Medium-wave infrared continuous zoom lens and imaging device - Google Patents

Medium-wave infrared continuous zoom lens and imaging device Download PDF

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CN111367064B
CN111367064B CN201811591878.1A CN201811591878A CN111367064B CN 111367064 B CN111367064 B CN 111367064B CN 201811591878 A CN201811591878 A CN 201811591878A CN 111367064 B CN111367064 B CN 111367064B
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lens
zoom lens
meniscus
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wave infrared
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CN111367064A (en
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张新
刘涛
王灵杰
史广维
张建萍
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Changchun Institute of Optics Fine Mechanics and Physics of CAS
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Changchun Institute of Optics Fine Mechanics and Physics of CAS
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    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B15/00Optical objectives with means for varying the magnification
    • G02B15/14Optical objectives with means for varying the magnification by axial movement of one or more lenses or groups of lenses relative to the image plane for continuously varying the equivalent focal length of the objective
    • G02B15/16Optical objectives with means for varying the magnification by axial movement of one or more lenses or groups of lenses relative to the image plane for continuously varying the equivalent focal length of the objective with interdependent non-linearly related movements between one lens or lens group, and another lens or lens group
    • G02B15/163Optical objectives with means for varying the magnification by axial movement of one or more lenses or groups of lenses relative to the image plane for continuously varying the equivalent focal length of the objective with interdependent non-linearly related movements between one lens or lens group, and another lens or lens group having a first movable lens or lens group and a second movable lens or lens group, both in front of a fixed lens or lens group
    • G02B15/167Optical objectives with means for varying the magnification by axial movement of one or more lenses or groups of lenses relative to the image plane for continuously varying the equivalent focal length of the objective with interdependent non-linearly related movements between one lens or lens group, and another lens or lens group having a first movable lens or lens group and a second movable lens or lens group, both in front of a fixed lens or lens group having an additional fixed front lens or group of lenses
    • G02B15/173Optical objectives with means for varying the magnification by axial movement of one or more lenses or groups of lenses relative to the image plane for continuously varying the equivalent focal length of the objective with interdependent non-linearly related movements between one lens or lens group, and another lens or lens group having a first movable lens or lens group and a second movable lens or lens group, both in front of a fixed lens or lens group having an additional fixed front lens or group of lenses arranged +-+

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Abstract

本发明公开了一种中波红外连续变焦镜头,其中,从物方到像方同轴依次排列前固定组、变焦透镜组、补偿透镜组、后固定组以及二次成像透镜组,所述前固定组具有正光焦度,所述变焦透镜组具有负光焦度,所述补偿透镜组具有正光焦度,所述后固定组具有正光焦度,所述二次成像透镜组具有正光焦度,所述变焦透镜组和所述补偿透镜组可轴向移动实现连续变焦。该中波红外连续变焦镜头,结构紧凑,满足冷光阑效率100%;所述变焦透镜组和所述补偿透镜组的轴向移动实现系统的连续变焦,变焦行程短且曲线平滑,在全焦范围内具有良好的成像质量。

Figure 201811591878

The invention discloses a mid-wave infrared continuous zoom lens, wherein a front fixed group, a zoom lens group, a compensation lens group, a rear fixed group and a secondary imaging lens group are coaxially arranged in sequence from the object side to the image side, the front fixed group The fixed group has positive refractive power, the zoom lens group has negative refractive power, the compensation lens group has positive refractive power, the rear fixed group has positive refractive power, and the secondary imaging lens group has positive refractive power, The zoom lens group and the compensation lens group can move axially to realize continuous zooming. The mid-wave infrared continuous zoom lens has a compact structure and satisfies 100% efficiency of the cold diaphragm; the axial movement of the zoom lens group and the compensation lens group realizes the continuous zoom of the system, the zoom stroke is short and the curve is smooth, and it can be used in the full focal range. Inside has good imaging quality.

Figure 201811591878

Description

Medium-wave infrared continuous zoom lens and imaging device
Technical Field
The invention relates to the technical field of optical imaging, in particular to a medium-wave infrared continuous zoom lens and an imaging device.
Background
When the optical instrument is used in a large temperature range, the lens focal power can be changed due to the expansion with heat and contraction with cold of the lens barrel material and the optical material and the temperature refractive index coefficient of the optical material, so that the defocusing phenomenon is generated, and the optical system can be defocused due to the expansion with heat and contraction with cold of the lens barrel material, so that the imaging quality is reduced. In order to reduce the influence of temperature variation on the imaging quality of the infrared optical system, a athermal design, or a thermal difference elimination design, is required, that is, through certain mechanical, optical, electronic and other technologies, defocusing caused by temperature variation is compensated, so that the infrared optical system keeps stable imaging quality in a temperature interval with a large variation range. The current heat difference eliminating mode mainly comprises the following steps: electromechanical active athermal differential, mechanical passive athermal differential, and optical passive athermal differential.
When the focal length of the infrared continuous zooming optical system is continuously changed in a certain range, the image surface is stable and good image quality can be kept. The size of the image surface scenery is continuously variable, and the visual effect which cannot be achieved by a fixed-focus lens and a multi-gear zoom lens can be achieved, so that the purposes of searching for a target with a large view field and carefully observing the target with a small view field are achieved.
At present, domestic research on a medium-wave infrared continuous zooming optical system has been reported in documents. Chinese patent publication No. CN106526818 discloses a three-group linked compact high zoom ratio infrared connection zoom optical system. However, the system adopts a three-component zooming mode, the optical system has a complex structure and higher control precision requirement, and the first compensation lens 3 is processed with an aspheric surface on a monocrystalline silicon material, so that the difficulty of optical processing is increased.
In summary, the three-component compact zoom lens has the problems of complex structure, difficult adjustment and the like; the aspheric surface on the monocrystalline silicon material increases the difficulty of optical processing.
Disclosure of Invention
The embodiment of the invention provides a medium-wave infrared continuous zoom lens and an imaging device, which can realize compact lens structure and have medium-wave infrared continuous zooming capability.
A first aspect provides a medium wave infrared continuous zoom lens, wherein a front fixed group, a zoom lens group, a compensation lens group, a rear fixed group and a secondary imaging lens group are coaxially and sequentially arranged from an object side to an image side, the front fixed group has positive focal power, the zoom lens group has negative focal power, the compensation lens group has positive focal power, the rear fixed group has positive focal power, the secondary imaging lens group has positive focal power, and the zoom lens group and the compensation lens group can axially move to realize continuous zooming.
With reference to the implementation manner of the first aspect:
the front fixed group is a meniscus silicon positive lens with a convex surface facing the object space, and the front surface and the rear surface of the meniscus silicon positive lens are spherical surfaces;
or the rear fixed group is a lens with a meniscus positive focal power, the convex surface of the lens faces the object space, and the front surface of the lens with the meniscus positive focal power is a diffraction surface processed on an even-order aspheric substrate;
or the compensation lens group comprises a first compensation lens and a second compensation lens which are coaxially and sequentially arranged from an object side to an image side, wherein the first compensation lens is a double convex positive lens, and the second compensation lens is a meniscus positive lens convex to the image side;
or the zoom lens group comprises a first zoom lens, a second zoom lens and a third zoom lens which are coaxially and sequentially arranged from an object side to an image side; the first zoom lens is a meniscus negative lens convex to the object, the second zoom lens is a meniscus positive lens convex to the object, and the third zoom lens is a biconcave negative lens;
or the secondary imaging lens group comprises a first meniscus lens with positive focal power convex to the image side and a second meniscus lens with positive focal power convex to the image side and positioned on the image side of the first meniscus lens.
With reference to the implementation manner of the first aspect:
the front surface of the first zoom lens is an even-order aspheric surface, and the rear surface of the first zoom lens is a spherical surface; the front surface and the rear surface of the second zoom lens are spherical surfaces; the front surface of the third zoom lens is a spherical surface, and the rear surface of the third zoom lens is an even-order aspheric surface;
or, the first variable focus lens is made of a germanium material, the second variable focus lens is made of a silicon material, and the third variable focus lens is made of a germanium material.
With reference to the implementation manner of the first aspect:
the front surface and the rear surface of the first compensation lens are spherical surfaces; the front surface of the second compensation lens is a spherical surface, and the rear surface of the second compensation lens is an even-order aspheric surface;
or the first compensation lens is made of a silicon material, and the second compensation lens is made of a zinc selenide material.
With reference to the implementation manner of the first aspect:
the front surface side surface of the first meniscus lens is a diffraction surface processed on an even-order aspheric substrate, and the rear surface of the first meniscus lens is a spherical surface; the front surface of the second meniscus lens is an even aspheric surface, and the rear surface of the second meniscus lens is a spherical surface;
or, the first meniscus lens and the second meniscus lens are both germanium lenses.
With reference to the implementation manner of the first aspect, the equation of the even aspheric surface is:
Figure BDA0001920460510000031
in the formula, Z is a distance rise from a vertex of the aspherical surface when the aspherical surface is at a position having a height h in the optical axis direction. c is 1/r, r represents the radius of curvature of the mirror surface, k is conic coefficient, and A, B, C, D is a high-order aspheric coefficient.
With reference to the implementation manner of the first aspect:
the high-order aspheric coefficients of the equation for the front surface of the first zoom lens are: a is-7.45 e-06, B is-5.65 e-10, C is 1.17e-12, D is-9.43 e-16;
the high-order aspheric coefficients of the equation for the rear surface of the third zoom lens are: a is-4.90 e-06, B is-1.39 e-10, C is 5.19e-12, D is-7.96 e-15;
the high-order aspheric coefficients of the equation for the rear surface of the second compensation lens are: a is 1.10e-06, B is 2.76e-10, C is-1.38 e-12, D is 2.28 e-15;
the high-order aspheric coefficients of the equation for the front surface of the lens of positive meniscus power are: a is-2.23 e-07, B is-1.70 e-08, C is 7.71e-11, D is-2.15 e-13;
the high-order aspheric surface coefficient of the even-order aspheric surface equation of the first meniscus lens is as follows: a is-1.94 e-04, B is 3.26e-06, C is-1.10 e-06, D is 3.24 e-08;
the high-order aspheric surface coefficient of the even-order aspheric surface equation of the second meniscus lens is as follows: a is-9.9 e-05, B is 9.09e-07, C is-6.11 e-09, and D is-4.50 e-12.
With reference to the implementation manner of the first aspect, the equation of the diffraction surface is:
φ(h)=α1h22h4
wherein alpha is1、α2Is the diffraction coefficient.
With reference to the implementation manner of the first aspect:
the diffraction coefficient of the equation for the diffractive surface of the front surface of the rear fixed set of lenses of positive meniscus power is: alpha is alpha1Is-1.48 e-04, alpha2Is-2.19 e-07;
the diffraction coefficient of the equation for the diffractive surface of the first meniscus lens is: alpha is alpha1Is-1.17 e-03, alpha2Is 5.23 e-06.
A second aspect provides an imaging device, which includes the above-mentioned medium wave infrared zoom lens and a medium wave infrared detector for receiving the image formed by the medium wave infrared zoom lens.
The invention has the beneficial effects that: the medium-wave infrared continuous zoom lens has a compact structure and meets the cold diaphragm efficiency of 100%; the axial movement of the zoom lens group and the compensation lens group realizes the continuous zooming of the system, the zooming stroke is short, the curve is smooth, and the imaging quality is good in the full-focus range.
Drawings
In order to more clearly illustrate the technical solutions in the embodiments of the present invention, the drawings needed to be used in the description of the embodiments will be briefly introduced below, and it is obvious that the drawings in the following description are only some embodiments of the present invention, and it is obvious for those skilled in the art to obtain other drawings based on these drawings without creative efforts. Wherein:
fig. 1 is a schematic view of a telephoto path of the medium-wave infrared continuous zoom lens according to the embodiment of the invention.
Fig. 2 is a schematic diagram of a middle focus optical path of the medium-wave infrared continuous zoom lens according to the embodiment of the present invention.
FIG. 3 is a schematic short-focus optical path diagram of the medium-wave infrared continuous zoom lens according to the embodiment of the present invention.
FIG. 4 is a graph of MTF at 20 ℃ in telephoto for the intermediate wave infrared continuous zoom lens according to the embodiment of the present invention.
FIG. 5 is a MTF curve diagram of the mid-focus of the mid-wave infrared continuous zoom lens according to the embodiment of the present invention at 20 ℃.
FIG. 6 is a MTF curve under 20 ℃ of short focus for the middle-wave infrared continuous zoom lens according to the embodiment of the present invention.
FIG. 7 is a MTF curve under a condition of tele-40 ℃ of the intermediate-wave infrared continuous zoom lens according to the embodiment of the present invention.
FIG. 8 is a MTF curve diagram of the intermediate focus of the intermediate wave infrared continuous zoom lens according to the embodiment of the present invention at-40 ℃.
FIG. 9 is a MTF curve under the condition of-40 ℃ short focus of the intermediate wave infrared continuous zoom lens according to the embodiment of the present invention.
FIG. 10 is a graph of MTF at 80 ℃ in telephoto for the intermediate wave infrared continuous zoom lens according to the embodiment of the present invention.
FIG. 11 is a MTF curve diagram of the mid-focus of the mid-wave infrared continuous zoom lens according to the embodiment of the present invention at 80 ℃.
FIG. 12 is a MTF curve graph at 80 ℃ for short focus of the mid-wave infrared continuous zoom lens according to the embodiment of the present invention.
Detailed Description
The technical solutions in the embodiments of the present invention will be clearly and completely described below with reference to the drawings in the embodiments of the present invention, and it is obvious that the described embodiments are only a part of the embodiments of the present invention, and not all of the embodiments. All other embodiments, which can be derived by a person skilled in the art from the embodiments given herein without making any creative effort, shall fall within the protection scope of the present invention.
Fig. 1 is a schematic view of a telephoto path of the medium-wave infrared continuous zoom lens according to the embodiment of the invention. Fig. 2 is a schematic diagram of a middle focus optical path of the medium-wave infrared continuous zoom lens according to the embodiment of the present invention. FIG. 3 is a schematic short-focus optical path diagram of the medium-wave infrared continuous zoom lens according to the embodiment of the present invention. For convenience of explanation, only portions related to the present invention are shown in the drawings. Referring to fig. 1, 2 and 3, the medium wave infrared continuous zoom lens according to the embodiment of the present invention includes a front fixed group 110, a zoom lens group 120, a compensation lens group 130, a rear fixed group 140 and a secondary imaging lens group 150 coaxially and sequentially arranged from an object side to an image side, wherein the front fixed group 110 has positive focal power, the zoom lens group 120 has negative focal power, the compensation lens group 130 has positive focal power, the rear fixed group 140 has positive focal power, the secondary imaging lens group 150 has positive focal power, and the zoom lens group 120 and the compensation lens group 130 are axially movable to achieve continuous zooming. In the field of optical lens technology, it is a common technique how to implement moving zooming/focusing, for example, the zoom lens group 120 and the compensation lens group 130 can be mounted on a slidable or rolling track or device, and the moving or moving can be implemented by a stepping motor or other power device, therefore, the detailed description will not be provided in this section.
The medium wave infrared continuous zoom lens provided by the embodiment of the invention adopts five groups of lenses, has simple and reasonable structural design and very compact volume, meets the requirement of 100% of cold diaphragm efficiency, realizes continuous zooming of a system by the axial movement of the zoom lens group and the compensation lens group, has short zooming stroke and smooth curve, has good imaging quality in a full focus range, and is beneficial to batch production of lenses.
The lens group described in the present invention may be a single lens in this embodiment or other embodiments, or may be a lens group composed of several lenses. According to the direction of the light path, the left side surface of all optical elements in the diagram is defined as a front surface, and the right side surface of all optical elements in the diagram is defined as a rear surface; the left side is defined as the object side, and the right side is defined as the image side.
Specifically, this embodiment preferably:
the front fixed group 110 is a positive meniscus silicon lens 110 with a convex surface facing the object, the front fixed group 110 is a fixed lens, that is, the position of the positive meniscus silicon lens 110 in the lens is fixed, and the mid-wave infrared light is converged by the positive meniscus silicon lens 110. The front and rear surfaces of the positive meniscus silicon lens 110 are spherical. The meniscus silicon positive lens 110 is further preferably made of silicon crystal material, which is convenient for processing and production and has stable optical quality.
The zoom lens group 120 includes a first zoom lens 121, a second zoom lens 122, and a third zoom lens 123 which are coaxially arranged in this order from the object side to the image side; the first zoom lens 121 is a meniscus negative lens convex toward the object, the second zoom lens 122 is a meniscus positive lens convex toward the object, and the third zoom lens 123 is a biconcave negative lens. Preferably, the front surface of the first zoom lens 121 is an even-order aspherical surface, and the rear surface is a spherical surface; the front and rear surfaces of the second zoom lens 122 are spherical; the front surface of the third zoom lens 123 is a spherical surface, and the rear surface is an even-order aspherical surface. The first variable focal length lens 121 is made of a germanium material, the second variable focal length lens 122 is made of a silicon material, and the third variable focal length lens 123 is made of a germanium material. The zoom lens group 120 is used for changing the focal length and the variable magnification of the medium-wave infrared continuous zoom lens. The moving stroke of the variable focus lens assembly 120 is 40.10mm, which satisfies the requirement of large-range zooming. All lens materials of the variable focus lens group 120 are crystal materials, so that the processing and the production are convenient, and the optical quality is stable.
The compensation lens group 130 includes a first compensation lens 131 and a second compensation lens 132 coaxially arranged in order from an object side to an image side, the first compensation lens 131 is a double convex positive lens, and the second compensation lens 132 is a positive meniscus lens convex to the image side. The first compensation lens 131 is made of a silicon material, and the second compensation lens 132 is made of a zinc selenide material. The moving stroke of the compensation lens group 130 is 27.95mm, which satisfies the requirement of zooming in a larger range. The lens material of the biconvex positive lens 130 is preferably a crystalline material, which facilitates processing and production and has stable optical quality. The compensation lens group 130 is used for compensating the image plane position offset of the medium wave infrared continuous zoom lens in the zooming process.
The axial movement of the zoom lens group 120 and the compensation lens group 130 realizes the continuous zooming of the medium wave infrared continuous zoom lens, and the zooming stroke is short and the curve is smooth.
The rear fixed group 140 is a positive meniscus lens 140 with the convex surface facing the object, and the rear fixed group 140 is also a fixed lens group. The front surface of the positive meniscus lens 140 (i.e., the object side surface of the rear fixed group 140) is a diffractive surface machined on an even-order aspheric substrate, and the rear surface is spherical. The front surface has a base even-order aspheric surface and a diffractive surface machined on the base, so that the surface is constrained by both the even-order aspheric equation and the diffractive equation. The material of the positive meniscus lens 140 is preferably zinc sulfide or zinc selenide, and is further preferably zinc sulfide crystal material or zinc selenide crystal material, so that the processing and production are convenient, and the optical quality is stable.
After being focused by the front four groups of optical elements such as the meniscus silicon positive lens 110, the zoom lens group 120, the compensation lens group 130, the meniscus positive lens 140 and the like, the medium wave infrared light forms an intermediate image behind (i.e. on the image side) the meniscus positive lens 140; the secondary imaging lens group 150 is disposed behind the intermediate image. In the following detailed description, the intermediate image is preferably formed 17.90mm behind the meniscus positive lens 140, and the secondary imaging lens 150 set is disposed 2.60mm behind the intermediate image, which makes the medium wave infrared zoom lens structure more compact.
The secondary imaging lens group 150 includes a second meniscus lens 152 of positive power convex to the image side and a first meniscus lens 151 of positive power convex to the image side on the image side of the second meniscus lens 152. The first meniscus lens 151 and the second meniscus lens 152 are both germanium lenses, and further preferably germanium crystal lenses, which are convenient for processing and production and have stable optical quality. The front surface (i.e., the object side surface) of the first meniscus lens 151 is a diffractive surface machined on an even-order aspherical surface substrate (i.e., the front surface has a basic even-order aspherical surface and a diffractive surface machined on the basis), and the rear surface thereof is a spherical surface. The front surface (i.e., the object side surface) of the second meniscus lens 152 is an even-aspheric surface, and the rear surface thereof is a spherical surface. The secondary imaging lens group 150 can be used for focusing and compensating the drift of a focal plane in real time along with the temperature change, so that the heat dissipation difference of-40 ℃ to 80 ℃ is realized (the imaging definition can be still kept within the temperature range of-40 ℃ to 80 ℃), and therefore, the medium-wave infrared continuous zoom lens has good heat dissipation difference capacity and can also be called a compact heat dissipation difference medium-wave infrared continuous zoom lens.
In this embodiment, the lens uses nine lenses in total, the total optical length is only 172.3mm, all the lenses are made of crystal materials, and the diffraction surfaces of the rear fixed group 140 and the first meniscus lens 151 correct various aberrations well, so that the optical system has good quality, can zoom continuously within the range of 29.4mm to 470mm of focal length, and can realize compact thermal aberration elimination medium wave infrared continuous zooming high-definition imaging.
The aspheric surface of the lens is arranged on materials such as germanium, zinc selenide or zinc sulfide which are easy to carry out diamond single-point turning, the silicon lens in the optical system is spherical, the traditional optical cold machining grinding and polishing process can be adopted, and the machining difficulty is reduced.
The lens structure of the embodiment of the invention has simple and reasonable design and is beneficial to the batch production of the lens; the volume is very compact, and the applicability and the application range are greatly expanded.
The equation of the even aspheric surface related in the embodiment of the invention is as follows:
Figure BDA0001920460510000081
in the formula, Z is a distance rise from a vertex of the aspherical surface when the aspherical surface is at a position having a height h in the optical axis direction. c is 1/r, r represents the radius of curvature of the mirror surface, k is conic coefficient, and A, B, C, D is a high-order aspheric coefficient.
The equation for the diffraction surface involved in the embodiments of the present invention is:
φ(h)=α1h22h4
wherein alpha is1、α2Is the diffraction coefficient.
According to the above equation and the spherical equation, the parameters of the embodiment of the present invention are as follows:
table 1, optical structure parameters of the inventive examples:
Figure BDA0001920460510000091
Figure BDA0001920460510000101
table 2, aspherical coefficients of examples of the present invention (surface numbers are the same as in table 1):
Figure BDA0001920460510000102
table 3, diffraction surface coefficients of the inventive examples (surface numbers same as table 1):
Figure BDA0001920460510000103
the lens of the medium-wave infrared continuous zoom lens provided by the embodiment of the invention is compact and has the heat difference eliminating capability, and specific lens parameters are shown in a table 4.
TABLE 4 lens parameters
Figure BDA0001920460510000104
Figure BDA0001920460510000111
The embodiment of the invention uses five groups of nine lenses together, all the lenses are made of crystal materials, a secondary imaging light path design is adopted, the lens materials, the radius, the distance and the thickness parameters are reasonably matched, the total optical length is only 172.3mm, the structure is compact, the working wave band is 3.4-5.0 μm, the F number is constant and is 4.0, the heat dissipation difference is-40-80 ℃, the cold diaphragm efficiency is 100 percent, the continuous zooming can be realized within the range of 29.4-470 mm of the focal length, the good imaging quality is realized within the full focus range, and the refrigeration medium wave infrared detectors with the resolution of 640 multiplied by 512, the pixel size of 15 μm, 20 μm and the like can be simultaneously adapted.
Fig. 4-6 are Modulation Transfer Function curves for the 20 c position for the tele, mid and short focus positions of the preferred embodiment of the present invention, and fig. 7-12 are Modulation Transfer Function curves for the-40 c and 80 c positions for the tele, mid and short focus positions of the preferred embodiment of the present invention. In the figure, the horizontal axis represents spatial frequency, unit: wire pairs per millimeter (lp/mm); and the value of a longitudinal axis surface Modulation Transfer Function (MTF) is used for evaluating the imaging quality of the lens, the value range is 0 to 1.0, the higher the MTF curve is, the straighter the MTF curve is, the better the imaging quality of the lens is, and the stronger the reduction capability of the real image is. As can be seen from fig. 4 to 6, the lens according to the embodiment of the present invention has excellent imaging capability at various focal lengths. As can be seen from FIGS. 7-12, after the lens compensates the drift of the focal plane, the lens assembly can be ensured to clearly image on the whole imaging surface under the environment of-40 ℃ to 80 ℃, and the requirement of poor heat dissipation is met.
Another embodiment of the present invention provides an imaging apparatus, which includes the above-mentioned medium wave infrared zoom lens and a medium wave infrared detector for receiving images formed by the medium wave infrared zoom lens. The medium wave infrared detector converts the image formed by the medium wave infrared continuous zoom lens into an electric signal for subsequent processing, and intelligent processing is realized. The imaging device may be a camera, a pod, or some other device or apparatus.
Further, the medium wave infrared detector is preferably a refrigeration medium wave infrared detector with the resolution of 640 x 512 and the pixel size of 15 μm or 20 μm, so that the adaptability of the imaging device of the embodiment of the invention is improved, and the popularization and the application are facilitated.
The above description is only an embodiment of the present invention, and not intended to limit the scope of the present invention, and all modifications of equivalent structures and equivalent processes performed by the present specification and drawings, or directly or indirectly applied to other related technical fields, are included in the scope of the present invention.

Claims (8)

1.一种中波红外连续变焦镜头,其特征在于,从物方到像方同轴依次排列前固定组、变焦透镜组、补偿透镜组、后固定组以及二次成像透镜组,所述前固定组具有正光焦度,所述变焦透镜组具有负光焦度,所述补偿透镜组具有正光焦度,所述后固定组具有正光焦度,所述二次成像透镜组具有正光焦度,所述变焦透镜组和所述补偿透镜组可轴向移动实现连续变焦;1. A mid-wave infrared continuous zoom lens, characterized in that a front fixed group, a zoom lens group, a compensation lens group, a rear fixed group and a secondary imaging lens group are sequentially arranged coaxially from the object side to the image side, the front The fixed group has positive refractive power, the zoom lens group has negative refractive power, the compensation lens group has positive refractive power, the rear fixed group has positive refractive power, and the secondary imaging lens group has positive refractive power, The zoom lens group and the compensation lens group can move axially to realize continuous zooming; 所述前固定组为一个凸面向物方的弯月硅正透镜,所述弯月硅正透镜的前后表面均为球面;The front fixed group is a convex meniscus silicon positive lens facing the object, and the front and rear surfaces of the meniscus silicon positive lens are spherical surfaces; 所述后固定组为一个凸面向物方的弯月正光焦度的透镜,所述弯月正光焦度的透镜的前表面为加工在偶次非球面基底上的衍射表面;The rear fixing group is a lens with a positive meniscus refractive power that is convex toward the object, and the front surface of the lens with a positive meniscus refractive power is a diffractive surface processed on an even-order aspherical substrate; 所述补偿透镜组包括从物方到像方同轴依次排列的第一补偿透镜和第二补偿透镜,所述第一补偿透镜为双凸正透镜,所述第二补偿透镜为凸向像方的弯月正透镜;The compensation lens group includes a first compensation lens and a second compensation lens arranged coaxially from the object side to the image side, the first compensation lens is a biconvex positive lens, and the second compensation lens is convex toward the image side The meniscus positive lens; 所述变焦透镜组包括从物方到像方同轴依次排列的第一变焦透镜、第二变焦透镜和第三变焦透镜;所述第一变焦透镜为凸向物方的弯月负透镜,所述第二变焦透镜为凸向物方的弯月正透镜,所述第三变焦透镜为双凹负透镜;The zoom lens group includes a first zoom lens, a second zoom lens and a third zoom lens that are coaxially arranged from the object side to the image side; the first zoom lens is a meniscus negative lens convex to the object side, so The second zoom lens is a meniscus positive lens convex to the object side, and the third zoom lens is a double concave negative lens; 所述二次成像透镜组包括凸向像方的正光焦度的第一弯月透镜和位于所述第一弯月透镜像方侧的凸向像方的正光焦度的第二弯月透镜;The secondary imaging lens group comprises a first meniscus lens with positive refractive power convex toward the image side and a second meniscus lens located on the image side of the first meniscus lens with positive refractive power convex toward the image side; 所述第一变焦透镜的前表面为偶次非球面,后表面是球面;所述第二变焦透镜的前后表面均为球面;所述第三变焦透镜的前表面为球面,后表面为偶次非球面;The front surface of the first zoom lens is an even-order aspheric surface, and the rear surface is a spherical surface; the front and rear surfaces of the second zoom lens are spherical surfaces; the front surface of the third zoom lens is a spherical surface, and the rear surface is an even-order surface. Aspherical; 所述第一变焦透镜的材料为锗材料,所述第二变焦透镜的材料为硅材料,所述第三变焦透镜的材料为锗材料;The material of the first zoom lens is germanium material, the material of the second zoom lens is silicon material, and the material of the third zoom lens is germanium material; 所述变焦透镜组的移动行程为40.10mm。The moving stroke of the zoom lens group is 40.10 mm. 2.根据权利要求1所述的中波红外连续变焦镜头,其特征在于:2. medium wave infrared continuous zoom lens according to claim 1, is characterized in that: 所述第一补偿透镜的前后表面均为球面;所述第二补偿透镜的前表面为球面,后表面为偶次非球面;The front and rear surfaces of the first compensation lens are spherical; the front surface of the second compensation lens is a spherical surface, and the rear surface is an even-order aspheric surface; 或者,所述第一补偿透镜的材料为硅材料,所述第二补偿透镜的材料为硒化锌材料。Alternatively, the material of the first compensation lens is silicon material, and the material of the second compensation lens is zinc selenide material. 3.根据权利要求1所述的中波红外连续变焦镜头,其特征在于:3. medium wave infrared continuous zoom lens according to claim 1, is characterized in that: 所述第一弯月透镜的前表面侧表面为加工在偶次非球面基底上的衍射表面,后表面为球面;所述第二弯月透镜的前表面为偶次非球面,后表面为球面;The front surface side surface of the first meniscus lens is a diffractive surface processed on an even-order aspherical substrate, and the rear surface is a spherical surface; the front surface of the second meniscus lens is an even-order aspherical surface, and the rear surface is a spherical surface ; 或者,所述第一弯月透镜和第二弯月透镜均为锗透镜。Alternatively, both the first meniscus lens and the second meniscus lens are germanium lenses. 4.根据权利要求1至3中任一一项所述的中波红外连续变焦镜头,其特征在于,所述偶次非球面的方程为:4. The mid-wave infrared continuous zoom lens according to any one of claims 1 to 3, wherein the equation of the even-order aspheric surface is:
Figure FDA0003181271610000021
Figure FDA0003181271610000021
式中,Z为非球面沿光轴方向在高度为h的位置时,距非球面顶点的距离矢高,c=1/r,r表示镜面的曲率半径,k为圆锥系数conic,A、B、C、D为高次非球面系数。In the formula, Z is the distance vector height from the vertex of the aspheric surface when the aspheric surface is at a position of height h along the optical axis, c=1/r, r is the radius of curvature of the mirror surface, k is the conic coefficient, A, B, C and D are high-order aspheric coefficients.
5.根据权利要求4所述的中波红外连续变焦镜头,其特征在于:5. medium wave infrared continuous zoom lens according to claim 4, is characterized in that: 所述第一变焦透镜的前表面的方程的高次非球面系数为:A为-7.45e-06,B为-5.65e-10,C为1.17e-12,D为-9.43e-16;The high-order aspheric coefficient of the equation of the front surface of the first zoom lens is: A is -7.45e-06, B is -5.65e-10, C is 1.17e-12, and D is -9.43e-16; 所述第三变焦透镜的后表面的方程的高次非球面系数为:A为-4.90e-06,B为-1.39e-10,C为5.19e-12,D为-7.96e-15;The higher-order aspheric coefficient of the equation of the rear surface of the third zoom lens is: A is -4.90e-06, B is -1.39e-10, C is 5.19e-12, and D is -7.96e-15; 所述第二补偿透镜的后表面的方程的高次非球面系数为:A为1.10e-06,B为2.76e-10,C为-1.38e-12,D为2.28e-15;The higher-order aspheric coefficient of the equation of the back surface of the second compensation lens is: A is 1.10e-06, B is 2.76e-10, C is -1.38e-12, and D is 2.28e-15; 所述后固定组的弯月正光焦度的透镜的前表面的方程的高次非球面系数为:A为-2.23e-07,B为-1.70e-08,C为7.71e-11,D为-2.15e-13;The higher-order aspheric coefficients of the equation of the front surface of the lens with the positive power of the meniscus of the rear fixed group are: A is -2.23e-07, B is -1.70e-08, C is 7.71e-11, D is -2.15e-13; 所述第一弯月透镜的偶次非球面的方程的高次非球面系数为:A为-1.94e-04,B为3.26e-06,C为-1.10e-06,D为3.24e-08;The higher-order aspheric coefficients of the equation of the even-order aspheric surface of the first meniscus lens are: A is -1.94e-04, B is 3.26e-06, C is -1.10e-06, and D is 3.24e- 08; 所述第二弯月透镜的偶次非球面的方程的高次非球面系数为:A为-9.9e-05,B为9.09e-07,C为-6.11e-09,D为-4.50e-12。The higher-order aspheric coefficients of the equation of the even-order aspheric surface of the second meniscus lens are: A is -9.9e-05, B is 9.09e-07, C is -6.11e-09, and D is -4.50e -12. 6.根据权利要求3所述的中波红外连续变焦镜头,其特征在于,所述衍射表面的方程为:6. The medium-wave infrared continuous zoom lens according to claim 3, wherein the equation of the diffractive surface is: φ(h)=α1h22h4…;φ(h)=α 1 h 22 h 4 …; 其中,α1、α2为衍射系数。Among them, α 1 and α 2 are diffraction coefficients. 7.根据权利要求6所述的中波红外连续变焦镜头,其特征在于:7. medium wave infrared continuous zoom lens according to claim 6, is characterized in that: 所述后固定组的弯月正光焦度的透镜的前表面的衍射表面的方程的衍射系数为:α1为-1.48e-04,α2为-2.19e-07;The diffraction coefficient of the equation of the diffraction surface of the front surface of the lens with the positive meniscus refractive power of the rear fixed group is: α 1 is -1.48e-04, and α 2 is -2.19e-07; 所述第一弯月透镜的衍射表面的方程的衍射系数为:α1为-1.17e-03,α2为5.23e-06。The diffraction coefficient of the equation of the diffractive surface of the first meniscus lens is: α 1 is -1.17e-03, and α 2 is 5.23e-06. 8.一种成像装置,其特征在于,包括权利要求1至7任一项所述的中波红外连续变焦镜头和用于接收所述中波红外连续变焦镜头所成像的中波红外探测器。8 . An imaging device, characterized in that it comprises the mid-wave infrared continuous zoom lens according to any one of claims 1 to 7 and a mid-wave infrared detector for receiving images from the mid-wave infrared continuous zoom lens. 9 .
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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2011053526A (en) * 2009-09-03 2011-03-17 Kinoshita Optical Research Institute Co Ltd Zoom lens
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